numeric-prelude-0.2: src/MathObj/Gaussian/Variance.hs
{-# LANGUAGE NoImplicitPrelude #-}
{-
We represent a Gaussian bell curve in terms of the reciprocal of its variance
and its value at the origin.
We could do some projective geometry in the exponent
in order to also have zero variance,
which corresponds to the dirac impulse.
-}
module MathObj.Gaussian.Variance where
import qualified MathObj.Polynomial as Poly
import qualified Algebra.Transcendental as Trans
import qualified Algebra.Algebraic as Algebraic
import qualified Algebra.Field as Field
import qualified Algebra.Absolute as Absolute
import qualified Algebra.Ring as Ring
import qualified Algebra.Additive as Additive
{-
import Algebra.Transcendental (pi, )
import Algebra.Ring ((*), (^), )
import Algebra.Additive ((+))
-}
import Test.QuickCheck (Arbitrary, arbitrary, )
import Control.Monad (liftM2, )
-- import Prelude (($))
import NumericPrelude.Numeric
import NumericPrelude.Base
data T a = Cons {amp, c :: a}
deriving (Eq, Show)
instance (Absolute.C a, Arbitrary a) => Arbitrary (T a) where
arbitrary =
liftM2 Cons
arbitrary
(fmap ((1+) . abs) arbitrary)
constant :: Ring.C a => T a
constant = Cons one zero
{-# INLINE evaluate #-}
evaluate :: (Trans.C a) =>
T a -> a -> a
evaluate f x =
sqrt (amp f) * exp (-pi * c f * x^2)
exponentPolynomial :: (Additive.C a) =>
T a -> Poly.T a
exponentPolynomial f =
Poly.fromCoeffs [zero, zero, c f]
norm1 :: (Algebraic.C a, Absolute.C a) => T a -> a
norm1 f =
sqrt $ abs (amp f) / c f
norm2 :: (Algebraic.C a, Absolute.C a) => T a -> a
norm2 f =
sqrt $ abs (amp f) / (sqrt $ 2 * c f)
normP :: (Trans.C a, Absolute.C a) => a -> T a -> a
normP p f =
sqrt (abs (amp f)) * (p * c f) ^? (- recip (2*p))
variance :: (Trans.C a) =>
T a -> a
variance f =
recip $ c f * 2*pi
multiply :: (Ring.C a) =>
T a -> T a -> T a
multiply f g =
Cons (amp f * amp g) (c f + c g)
{- |
> convolve x y t =
> integrate $ \s -> x s * y(t-s)
-}
convolve :: (Field.C a) =>
T a -> T a -> T a
convolve f g =
Cons
(amp f * amp g / (c f + c g))
(recip $ recip (c f) + recip (c g))
{- |
> fourier x f =
> integrate $ \t -> x t * cis (-2*pi*t*f)
-}
fourier :: (Field.C a) =>
T a -> T a
fourier f =
Cons (amp f / c f) (recip $ c f)
{-
fourier (t -> exp(-(a*t)^2))
-}
dilate :: (Field.C a) => a -> T a -> T a
dilate k f =
Cons (amp f) $ c f / k^2
shrink :: (Ring.C a) => a -> T a -> T a
shrink k f =
Cons (amp f) $ c f * k^2
amplify :: (Ring.C a) => a -> T a -> T a
amplify k f =
Cons (k^2 * amp f) $ c f
{- laws
fourier (convolve f g) = multiply (fourier f) (fourier g)
dilate k (dilate m f) = dilate (k*m) f
dilate k (shrink k f) = f
variance (dilate k f) = k^2 * variance f
variance (convolve f g) = variance f + variance g
-}